Bifurcation And Chaos In Nonsmooth Mechanical Systems, Series A, Vol. 45

In order to study the behaviour of a mechanical system consisting of a cable with its shaft, a gear lever and its support (see in Fig. 12.1) we introduce a simplified seven degrees of freedom (DOF) system. An equivalent mass m with displacement X 4 and clearance ? exhibits impact nonlinearity due to the motor (see Fig. 12.2). Though a real physical external excitation would be more complex, we only consider a simple form of excitation u(t)= ?sin ( ?t) with amplitude ? and frequency ?.
The cable is represented by a mass M 1 with displacement X 5 and equivalent stiffness k 1 (see Fig. 12.2): this is a one DOF reduction of the continuous system. Impacts between m and M 1 are governed by a classical restitution law with coefficient e. The displacements of masses m and M 1 are governed by the equations:
| (12.1) | |
| (12.2) | |
The functions X 4 and X 5 remain smooth if X 4 ? X 5 ?] ? ?, ?[. Elastic impacts occur if X 4 ? X 5= ?. Using some algebra (related to momentum conservation [Brogliato (1996)]) velocities
and
after an impact are given by the relations:
| (12.3) | |
where
and